Experimental Study of Initial Fuel Temperature on the Burning Rates of Kerosene Pools in Cold Environment

2015 ◽  
Vol 4 (1) ◽  
pp. 36-39
Author(s):  
Kunal Ahuja ◽  
Alagani Harish ◽  
Vasudevan Raghavan
2019 ◽  
Vol 201 ◽  
pp. 93-103 ◽  
Author(s):  
Chen Kuang ◽  
Longhua Hu ◽  
Xiaolei Zhang ◽  
Yujie Lin ◽  
Larry W. Kostiuk

2007 ◽  
Vol 18 (3) ◽  
pp. 177-185 ◽  
Author(s):  
Timothy F. Platts-Mills ◽  
Eric Stendell ◽  
Matthew R. Lewin ◽  
Micheal N. Moya ◽  
Kulraj Dhah ◽  
...  

Trudy NAMI ◽  
2021 ◽  
pp. 74-86
Author(s):  
G. G. Ter-Mkrtich'yan

Introduction (problem statement and relevance). Hydrocarbon emissions from vaporizationtank fuel contribute significantly to the total emissions of hazardous substances from vehicles equipped with spark ignition engines. To meet the established standards for limiting hydrocarbon emissions caused by evaporation, all modern vehicles use fuel vapor recovery systems, the optimal parameters of which require the availability and application of mathematical models and methods for their determination.The purpose of the research was to develop a model of vapor generation processes in the car fuel tank and a methodology for determining the main quantitative parameters of the vapor-air mixture.Methodology and research methods. The analysis of the processes of vapor generation in the fuel tank was carried out. It was shown that the mass of hydrocarbons generated in the steam space was directly proportional to its volume and did not depend on the amount of fuel in the tank.Scientific novelty and results. New analytical dependences of the vaporization amount on the saturated vapor pressure, barometric pressure, initial fuel temperature and fuel heating during parking have been obtained.Practical significance. A formula was obtained to estimate the temperature of gasoline boiling starting in the tank, depending on the altitude above sea level and the volatility of gasoline, determined by the pressure of saturated vapors. Using the new equations, the vaporization analysis in real situations (parking, idling, refueling, explosive concentration of vapors) was carried out.


2018 ◽  
Vol 31 (5) ◽  
pp. 436-449 ◽  
Author(s):  
Depeng Kong ◽  
Zhen Zhang ◽  
Ping Ping ◽  
Xu He ◽  
Hanbing Yang

2013 ◽  
Vol 185 (3) ◽  
pp. 408-419 ◽  
Author(s):  
Stefan Schälike ◽  
Hyunjoo Chun ◽  
Kirti Bhushan Mishra ◽  
Klaus-Dieter Wehrstedt ◽  
Axel Schönbucher

2020 ◽  
Author(s):  
Daisuke Kawano ◽  
Kentaro Tsukiji ◽  
Hiroki Saito ◽  
Dai Matsuda ◽  
Eriko Matsumura ◽  
...  

2014 ◽  
Vol 1016 ◽  
pp. 587-591 ◽  
Author(s):  
Man Hou Li ◽  
Shou Xiang Lu ◽  
Jin Guo ◽  
Kwok Leung Tsui

Flame spreading over liquid fuels is a common phenomenon involving in accidental fuel leakage in aircraft crash or oil tanker which may result in many casualties and economic losses. Comparative experiments are conducted concerning flame spread over aviation kerosene (RP5) and 0# diesel at a variety of initial fuel temperatures. The threshold value of initial fuel temperature for liquid-phase and gas-phase controlled flame spread is approximately 17 °C larger than liquid’s flashpoint for both oils. For a given initial fuel temperature, due to low volatility and ignitability of 0# diesel, its flame spread rate is smaller than that of RP5, while the length of the horizontal subsurface convection flow is larger. Given the difference in flame speed, fire accidents for RP5 are potentially more hazardous than those of 0# diesel. Moreover, the variation trend of subsurface convection flow length falls nearly linearly with the initial fuel temperature for both fuels.


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